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hamiltonian [2016/09/08 22:46] nikolaj |
hamiltonian [2016/09/08 22:48] nikolaj |
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| $u = w + \Delta_{wu}$ | $u = w + \Delta_{wu}$ | ||
| - | the evolution is described by individually non-measurable oscillations ${\mathrm e}^{-iw}$ resp. ${\mathrm e}^{-iv}$ and, given we can rescale $w$ e.g. to $2\pi$, what's interesting is ${\mathrm e}^{-i\Delta_{wu}}$, capturing how much faster the second state oscillates. | + | the evolution is described by individually non-measurable oscillations ${\mathrm e}^{-iw}$ resp. ${\mathrm e}^{-iu}={\mathrm e}^{-iw}{\mathrm e}^{-i\Delta_{wu}}$ and what's interesting is the second factor, capturing how much faster the second state oscillates. |
| - | == Superposition state == | + | == Superposition states == |
| For | For | ||
